Critical field

For a given temperature, the critical field refers to the maximum magnetic field strength below which a material remains superconducting. Superconductivity is characterized both by perfect conductivity (zero resistance) and by the complete expulsion of magnetic fields (the Meissner effect). Changes in either temperature or magnetic flux density can cause the phase transition between normal and superconducting states.[1] The highest temperature under which the superconducting state is seen is known as the critical temperature. At that temperature even the weakest external magnetic field will destroy the superconducting state, so the strength of the critical field is zero. As temperature decreases, the critical field increases generally to a maximum at absolute zero.

For a type-I superconductor the discontinuity in heat capacity seen at the superconducting transition is generally related to the slope of the critical field ( $H_{\text{c}}$ ) at the critical temperature ( $T_{\text{c}}$ ):[2]

C_{\text{super}}-C_{\text{normal}}={T \over 4\pi }\left({\frac {dH_{\text{c}}}{dT}}\right)_{T=T_{\text{c}}}^{2}

There is also a direct relation between the critical field and the critical current – the maximum electric current density that a given superconducting material can carry, before switching into the normal state.[1] According to Ampère's law any electric current induces a magnetic field, but superconductors exclude that field. On a microscopic scale the magnetic field is not quite zero at the edges of any given sample – a penetration depth applies. For a type-I superconductor, the current must remain zero within the superconducting material (to be compatible with zero magnetic field), but can then go to non-zero values at the edges of the material on this penetration-depth length-scale, as the magnetic field rises.[2] As long as the induced magnetic field at the edges is less than the critical field, the material remains superconducting, but at higher currents the field becomes too strong and the superconducting state is lost. This limit on current density has important practical implications in applications of superconducting materials – despite zero resistance they cannot carry unlimited quantities of electric power.

The geometry of the superconducting sample complicates practical measurement of the critical field[2] – the critical field is defined for a cylindrical sample with the field parallel to the axis of radial symmetry. With other shapes (spherical, for example), there may be a mixed state with partial penetration of the exterior surface by the magnetic field (and thus partial normal state), while the interior of the sample remains superconducting.

Type-II superconductors allow a different sort of mixed state, where the magnetic field (above the lower critical field $H_{c1}$ ) is allowed to penetrate along cylindrical "holes" through the material, each of which carries a magnetic flux quantum. Along these flux cylinders the material is essentially in a normal, non-superconducting state, surrounded by superconductor where the magnetic field goes back to zero. The width of each cylinder is on the order of the penetration depth for the material. As the magnetic field increases, the flux cylinders move closer together and eventually at the upper critical field $H_{\text{c2}}$ , they leave no room for the superconducting state and the zero-resistivity property is lost.

Upper critical field

The upper critical field is the magnetic flux density (usually expressed with the unit tesla (T)) that completely suppresses superconductivity in a type-II superconductor at 0 K (absolute zero).

More properly, the upper critical field is a function of temperature (and pressure) and if these are not specified, absolute zero and standard pressure are implied.

Werthamer–Helfand–Hohenberg theory predicts the upper critical field ( $H c2$ ) at 0 K from $T c$ and the slope of $H c2$ at $T c$ .

The upper critical field (at 0 K) can also be estimated from the coherence length ( $ξ$ ) using the Ginzburg–Landau expression: $H c2$ = 2.07×10⁻¹⁵ T⋅m² $/(2 πξ 2)$ .[3]

Articles on superconductivity use $H c2$ or $B c2$ interchangeably since superconducting materials often exhibit perfect diamagnetism with susceptibility $χ = -1$ , resulting in equal magnitudes for $| H c2 |$ and $| B c2 |$ .

Lower critical field

The lower critical field is the magnetic flux density at which the magnetic flux starts to penetrate a type-II superconductor.

gollark: ZISCs are a lie because they generally have one instruction.

gollark: Reduced Instruction Set™ Computing™™

gollark: It seems like it would work, although maybe not be very RISCy, to have a stack stored out of the main linear memory with instructions to save and restore execution state.

gollark: I don't see how this "link register" thing works. What happens when you want to return twice?

gollark: They all run in the CLOUD™.

References

High Temperature Superconductivity, Jeffrey W. Lynn Editor, Springer-Verlag (1990)
Superconductivity of Metals and Alloys, P. G. de Gennes, Addison-Wesley (1989)
Introduction to Solid State Physics, Charles Kittel, John Wiley and Sons, Inc.

This article is issued from Wikipedia. The text is licensed under Creative Commons - Attribution - Sharealike. Additional terms may apply for the media files.

[LynnSuperconductivity-1] High Temperature Superconductivity, Jeffrey W. Lynn Editor, Springer-Verlag (1990)

[deGennes-2] Superconductivity of Metals and Alloys, P. G. de Gennes, Addison-Wesley (1989)

[3] Introduction to Solid State Physics, Charles Kittel, John Wiley and Sons, Inc.